TY - JOUR
T1 - Anisotropic magnetization and electronic structure of the first-order ferrimagnet ErCo2 studied by polarization dependent hard X-ray photoemission spectroscopy
AU - Abozeed, Amina A.
AU - Gorbunov, Denis I.
AU - Kadono, Toshiharu
AU - Kanai-Nakata, Yuina
AU - Yamagami, Kohei
AU - Fujiwara, Hidenori
AU - Sekiyama, Akira
AU - Higashiya, Atsushi
AU - Yamasaki, Atsushi
AU - Tamasaku, Kenji
AU - Yabashi, Makina
AU - Ishikawa, Tetsuya
AU - Wada, Hirofumi
AU - Andreev, Alexander V.
AU - Imada, Shin
N1 - Funding Information:
We are grateful to K. Kuga, M. Murata, S. Taniguchi, M. Iwano, C. Morimoto, K. Sakamoto, S. Fujioka, S. Hamamoto and K. Nakagawa for experimental supports. The HAXPES experiments were performed at BL19LXU of SPring-8 (Proposal No. 20150043). This work was supported by Materials Growth and Measurement Laboratory (https://mgml.eu) and by Project No. 21-09766S of the Czech Science Foundation. We acknowledge the support of HLD at HZDR, member of the European Magnetic Field Laboratory (EMFL). This work was also supported by a Grant in Aid for Scientific Research on Innovative Areas “J-Physics” (grant number JP16H01074) from MEXT, Japan and those for Scientific Researches (grant numbers JP16H04014, JP21K04869) from JSPS, Japan. A. Abozeed was supported by Otsuki memorial scholarship for Asian and African countries. Y. Kanai-Nakata was supported by the JSPS Research Fellowships for Young Scientists.
Funding Information:
We are grateful to K. Kuga, M. Murata, S. Taniguchi, M. Iwano, C. Morimoto, K. Sakamoto, S. Fujioka, S. Hamamoto and K. Nakagawa for experimental supports. The HAXPES experiments were performed at BL19LXU of SPring-8 (Proposal No. 20150043). This work was supported by Materials Growth and Measurement Laboratory ( https://mgml.eu ) and by Project No. 21-09766S of the Czech Science Foundation . We acknowledge the support of HLD at HZDR, member of the European Magnetic Field Laboratory (EMFL). This work was also supported by a Grant in Aid for Scientific Research on Innovative Areas “J-Physics” (grant number JP16H01074 ) from MEXT , Japan and those for Scientific Researches (grant numbers JP16H04014 , JP21K04869 ) from JSPS , Japan. A. Abozeed was supported by Otsuki memorial scholarship for Asian and African countries. Y. Kanai-Nakata was supported by the JSPS Research Fellowships for Young Scientists.
Publisher Copyright:
© 2022 The Authors
PY - 2023/1/15
Y1 - 2023/1/15
N2 - The first-order ferrimagnet ErCo2 attracts interest not only because of metamagnetism and magnetocaloric effect just above TC ≈ 32–34 K but also because it is closely related with the itinerant metamagnetism of YCo2 and LuCo2. We study the electronic structure of single crystals with hard X-ray photoemission spectroscopy (HAXPES). Magnetization measurements reconfirm the first-order magnetic transition, metamagnetism, and strong magnetic anisotropy. Calculated ErCo2 band structures of the ferrimagnetic and paramagnetic phases are presented in detail. In the ferrimagnetic state, the density of states just below EF is smaller than in the paramagnetic phase. Valence band spectra in the paramagnetic state show strong polarization dependence. Furthermore, the change across the first-order ferrimagnetic transition in the valence band electronic structures is observed. These experimental data are well described by the band structure calculation incorporated with the polarization dependent cross-sections of orbitals. We further discuss possible effects of electron correlation and spin fluctuation.
AB - The first-order ferrimagnet ErCo2 attracts interest not only because of metamagnetism and magnetocaloric effect just above TC ≈ 32–34 K but also because it is closely related with the itinerant metamagnetism of YCo2 and LuCo2. We study the electronic structure of single crystals with hard X-ray photoemission spectroscopy (HAXPES). Magnetization measurements reconfirm the first-order magnetic transition, metamagnetism, and strong magnetic anisotropy. Calculated ErCo2 band structures of the ferrimagnetic and paramagnetic phases are presented in detail. In the ferrimagnetic state, the density of states just below EF is smaller than in the paramagnetic phase. Valence band spectra in the paramagnetic state show strong polarization dependence. Furthermore, the change across the first-order ferrimagnetic transition in the valence band electronic structures is observed. These experimental data are well described by the band structure calculation incorporated with the polarization dependent cross-sections of orbitals. We further discuss possible effects of electron correlation and spin fluctuation.
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U2 - 10.1016/j.physb.2022.414465
DO - 10.1016/j.physb.2022.414465
M3 - Article
AN - SCOPUS:85141794866
SN - 0921-4526
VL - 649
JO - Physica B: Condensed Matter
JF - Physica B: Condensed Matter
M1 - 414465
ER -